Answer 1

1. Consider an object moving in an x-y plane. Let the initial velocity of the object be `vec"u"` at t = 0 and its velocity at time t be `vec"v"`
2. As the acceleration is constant, the average acceleration and the instantaneous acceleration will be equal.
   `vec"a"_"av" = (vec"v"_2 - vec"v"_1)/("t"_2 - "t"_1) = (("v"_"2x" - "v"_"1x")/("t"_2 - "t"_1))hat"i" + (("v"_"2y" - "v"_"1y")/("t"_2 - "t"_1))`
   ∴ `vec"a" = ((vec"v" - vec"u"))/(("t - 0"))`
   ∴ `vec"v" = vec"u" + vec"a""t"`      ....(1)
   This is the first equation of motion in vector form.
3. Let the displacement of the object from time t = 0 to t be `vec "s"`
   For constant acceleration, `vec"v"_"av" = (vec"v" + vec"u")/2`
   `vec"s" = (vec"v"_"av")"t" = ((vec"v" + vec"u")/2)"t" = ((vec"u" + vec"u" + vec"a""t")/2)"t"`
   ∴ `vec"s" = vec"u""t" + 1/2 vec"a""t"^2`   ...(2)
   This is the second equation of motion in vector form.
4. Equations (1) and (2) can be resolved into their x and y components so as to get corresponding scalar equations as follows.
   `"v"_"x" = "u"_"x" + "a"_"x" "t"`    ....(3)
   `"v"_"y" = "u"_"y" + "a"_"y" "t"`    ....(4)
   `"s"_"x" = "u"_"x" "t" + 1/2 "a"_"x""t"^2`   ...(5)
   `"s"_"y" = "u"_"y""t" + 1/2"a"_"y""t"^2`   ....(6)
5. It can be seen that equations (3) and (5) involve only the x components of displacement, velocity and acceleration while equations (4) and (6) involve only the y components of these quantities.
6. Thus, the motion along the x-direction of the object is completely controlled by the x components of velocity and acceleration while that along the y-direction is completely controlled by the y components of these quantities.
7. This shows that the two sets of equations are independent of each other and can be solved independently.